The hammer of mass M falls freely under the gravity through a distance. Let v be the speed acquired by the hammer when it strikes the rail obviously.
v =√gh ……… (1)
On impact, the hammer and rail are stuck together. Let v be the speed of the combination after impact. The law of conservation of momentum gives.
Mv = (M + m) v1 …….. (2)
Where m is the mass of the rail. Let FG be the average resistance (or resistive force) exerted by the ground. The net upward force F on the hammer rail combination is
F = FG – (M + m)g.
The combination moves through a distance ‘d’ against this net upward force. Obviously, the work done against the force F in a distance ‘d’ must equal to the kinetic energy the combination had just after impact.
\(\frac{1}{2}\) (M+m) v12 = F x d
= [FG – (M + m) g] × d ……… (3)
By equations (1) & (2), we can rewrite equation (3) as

2. Let the hammer rail combination be moving for a time Δt, before coming to rest. If ΔP is the change in momentum,
(Δp/Δt) = FG – (M + m)g
|Δp| = (M + m) v1 – 0

3. The kinetic energy of the hammer rail mcombination just before the impact is \(\frac{1}{2}\)(M +m) v2.
Mv2 and after impact, it is
Loss in kinetic energy = \(\frac{1}{2}\)Mv2 – \(\frac{1}{2}\).
